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    Table of ContentsTable of ContentsTable of ContentsTable of Contents

    Overview of CADNICA BatteriesOverview of CADNICA BatteriesOverview of CADNICA BatteriesOverview of CADNICA Batteries1-1. Advantages and Characteristics of CADNICA (Nickel-Cadmium) Batteries

    1-2. Theory of Operation, Manufacturing Processes and Structural Designs of CADNICA Batteries

    Charge CharacteristicsCharge CharacteristicsCharge CharacteristicsCharge Characteristics2-1. Outline of Charge Characteristics 2-2. Charge Efficiency 2-3. Cell Temperature during Charge2-4. Internal Gas Pressure during Charge 2-5. Cell Voltage during Charge

    Discharge CharacteristicsDischarge CharacteristicsDischarge CharacteristicsDischarge Characteristics3-1. Outline of Discharge Characteristics 3-2. Internal Resistance 3-3. Discharge Capacity

    3-4. Polarity Reversal

    Storage CharacteristicsStorage CharacteristicsStorage CharacteristicsStorage Characteristics4-1. General 4-2. Storage Conditions 4-3. Items to be Remembered for Storage

    Battery Service LifeBattery Service LifeBattery Service LifeBattery Service Life5-1. General 5-2. Factors Influencing Service Life 5-3. Summary of Service Life

    Special Purpose BatteriesSpecial Purpose BatteriesSpecial Purpose BatteriesSpecial Purpose Batteries6-1. High-capacity CADNICA Batteries 6-2. Fast-charge CADNICA Batteries

    6-3. High-temperature CADNICA Batteries 6-4. Heat-resistant CADNICA Batteries

    6-5. Memory-backup CADNICA Batteries

    CADNICA SLIMCADNICA SLIMCADNICA SLIMCADNICA SLIM7-1. Characteristics of CADNICA SLIM 7-2. Structure of CADNICA SLIM 7-3. Charge Characteristics

    7-4. Discharge Characteristics 7-5. Temperature Characteristics 7-6. Storage Characteristics

    7-7. Battery Service Life

    Charging Methods and Charging CircuitsCharging Methods and Charging CircuitsCharging Methods and Charging CircuitsCharging Methods and Charging Circuits8-1. Outline of Charging Methods 8-2. Charging Methods 8-3. Quick Charge

    8-4. Designing Charging Circuits 8-5. Parallel Charge and Parallel Discharge

    Assembled BatteryAssembled BatteryAssembled BatteryAssembled Battery9-1. Outline of Assembled Battery 9-2. How to Assemble Batteries 9-3. Interchangeability with Dry Cells

    General Remarks and PrecautionsGeneral Remarks and PrecautionsGeneral Remarks and PrecautionsGeneral Remarks and Precautions

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    1Overview ofOverview ofOverview ofOverview of

    CADNICACADNICACADNICACADNICA

    BatteriesBatteriesBatteriesBatteries1-1 Characteristics of

    CADNICA

    (Nickel-Cadmium)

    Batteries

    1-2 Theory of Operation,

    Manufacturing Processes

    and Structural Designs ofCADNICA Batteries

    1-11-11-11-1 Advantages andAdvantages andAdvantages andAdvantages and

    Characteristics of CADNICACharacteristics of CADNICACharacteristics of CADNICACharacteristics of CADNICA

    (Nickel-Ca(Nickel-Ca(Nickel-Ca(Nickel-Cadmium) Batteriesdmium) Batteriesdmium) Batteriesdmium) Batteries

    As an energy storage and conversion system,

    CADNICA batteries excel in ease of operation and

    electric characteristics, even though being classified

    as a secondary battery. Anticipating diversified

    market requirements, Sanyo Electric Co., L td. has

    put CADNICA batteries to use in sophisticated appli-

    cations that call for such requirements as high-speed

    charging and high-temperature operation, while

    maintaining all the features of general-use

    CADNICA batteries. Significant features of the

    CADNICA battery are as follows.

    (1) Outstanding economy and long service life which

    can last over 500 charge/discharge cycles.

    (2) Low internal resistance which enables high-rate

    discharge, and constant discharge voltage which

    guarantees excellent sources of DC power for any

    battery-operated appliance.

    (3) Sealed construction which prevents leakage of

    electrolyte and is maintenance free. No restric-

    tion on mounting direction so as to be incorpo-

    rated in any appliance.

    (4) Abil ity to withstand overcharge and overdischar-

    ge.

    (5) Long storage life without deterioration in perfor-

    mance; and recovery of normal performance on

    being recharged.

    (6) Operational within a wide temperature range.

    (7) Casing made from metal provides extra strength.

    (8) Similarities in discharge voltage betweenCADNICA and dry cells allow interchange

    ability.

    (9) High reliabil ity in performance due to high stan-

    dard quality control in manufacturing process

    based on ISO9000 standards.

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    1-1-1-1-2222 Theory of Operation,Theory of Operation,Theory of Operation,Theory of Operation,

    Manufacturing ProcessesManufacturing ProcessesManufacturing ProcessesManufacturing Processes andandandand

    Structural Designs ofStructural Designs ofStructural Designs ofStructural Designs of

    CADNICA BatteriesCADNICA BatteriesCADNICA BatteriesCADNICA Batteries

    1-1-1-1- 2222-1-1-1-1 Theory of OperationTheory of OperationTheory of OperationTheory of OperationAs its name suggests, the Nickel-Cadmium battery

    has a positive electrode made of nickel hydroxide and

    a negative electrode in which a cadmium compound is

    used as active material. Potassium hydroxide is used

    as its electrolyte. During change and discharge, the

    following reactions take place:

    (At the positive)

    Discharge

    NiOOHH2O + e Ni(OH)2+ OH

    Charge 0.52(1)

    (At the negative)

    Discharge

    Cd + 2OH

    d(

    )2 + 2e

    Charge 0.80(2)

    (Overall)

    Discharge

    2NiOOH + Cd + 2H2O 2Ni(OH)2+ Cd(OH)2

    Charge

    1.32(3)

    (Standard electromotive force)

    Namely, at the positive electrode, changes take place

    between nickel oxyhydroxide and nickel hydroxide,

    and at the negative electrode between cadmium

    metal and cadmium hydroxide.

    In Eq. (3) above, potassium hydroxide does not playa role in the electrochemical reaction of the Nickel-

    Cadmium battery apparently. In addition, it is a

    well-known fact that the H 2O molecules which are

    generated during charge disappear during discharge.

    Therefore, variations in electrolyte concentration are

    insignificant. Because of this reaction, the Nickel-

    Cadmium battery excels in temperature character-

    istics, high-rate discharge characteristics, durabil ity,

    etc. Most significant is the fact that the amount of

    electrolyte in a cell can be sizably reduced in order to

    allow completely sealed cells to be manufactured.

    With any other types of batteries, the discharged

    active materials will be exhausted as the batteries

    reach a fully charged state. Consequently, electrolysis

    of water contained in electrolyte commences. I t is

    well-known that at this stage oxygen and hydrogen

    gases begin to be generated respectively at the

    positive and negative electrodes. This will result in a

    decrease of water contained in electrolyte. At the

    same time, the gases will build up the internal

    pressure of a battery. Finally, the battery will be

    destroyed or electrolyte will run short, deteriorating

    the charge/discharge characteristics.

    Because of its unique design, the CADN ICA battery

    is capable of completely consuming the gases that

    evolve internally, extending its normal service life.

    Some of its notable design features are as follows:

    (1) Active materials have greater capacity at the

    negative than at the positive electrode.

    (2) The electrode used features superior conductivity

    and exemplary uniform distribution of its active

    materials.

    (3) The electrodes are thin plates having a large

    surface area. The negative and positive

    electrodes sandwich a separator through whichgases freely move. These are wound tightly and

    housed in the casing.

    (4) The electrolyte in a cell is kept to the precise

    quantity needed for the required output capacity.

    Fig.1-1 illustrates the charging process of the

    CADNICA battery. As shown in this process chart,

    the positive electrode becomes fully charged well

    before the negative electrode which is larger in

    capacity. Then, oxygen gas is generated by the

    electrolysis of water in the following manner.

    4OH 2H2O + O24e

    (4)

    Oxygen gas migrates to the negative electrode

    where it is recombined and removed from the gas

    phase.

    Thus, the negative electrode will not become fully

    charged and there will be no generation of hydrogen

    gas. Because cadmium reacts quickly to oxygen, they

    produce cadmium hydroxide at the negative electrode

    where cadmium metal is produced on charge. This

    takes the process described in Eq. (5).

    Gas Recombination

    Cd + 1/2O2+ H2O Cd(OH)2

    (5) ChargeCd(OH)2+ 2e

    Cd +2OH

    (2)

    The cadmium hydroxide produced by the process

    described in Eq. (5) is originally a discharge product

    of the negative electrode as is clear from Eq. (2). I f

    overcharge current is limited, the reaction rate in Eq.

    (5) will ultimately catch up with the reaction rate in

    Eq. (4) and a balance wil l be achieved. In other

    words, the apparent charging of the negative

    electrode will cease to continue any further. This

    means that the negative electrode will remain short

    of being fully charged all the time and the generationof hydrogen gas will not occur.

    Besides the chemical recombination mechanism of

    oxygen gas described above, oxygen gas is recom-

    bined electrochemically in the CADNICA battery.

    As explained previously, the CADNICA battery is

    composed of electrodes which have very large surface

    areas. These are placed side by side, sandwiching a

    separator which allows the free passage of gaseous

    substance. Accordingly, the oxygen gas generated at

    the positive electrode moves through the separator

    and reaches into the negative electrode, where it is

    quickly reduced due to the prevalent state of

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    potential. Consequently, at the boundaries of three

    phases namely oxygen gas (gas), electrolyte

    (liquid) and negative electrode (solids) the reac-

    tion shown in Eq. (6) takes place, causing oxygen gas

    to be recombined.

    2H2O + O2+ 4e 4OH

    (6)

    The CADNICA battery has a mechanism of

    completely disposing of the entire quantity of oxygengas generated in its sealed casing.

    Fig.1-1:Fig.1-1:Fig.1-1:Fig.1-1: Gas-Recombining MechanismGas-Recombining MechanismGas-Recombining MechanismGas-Recombining Mechanism

    of CADNICA Batteryof CADNICA Batteryof CADNICA Batteryof CADNICA Battery

    o2o2

    o2

    o2 o2 o2

    Positive

    Negative Negative Negative

    S epa rator

    Positive Positive

    Before fully charged(Charging reactionproceeds almostquantitatively.)

    After full charge,gas is generated.(Positive electrodeis fully charged.)

    Being overcharged,gas is consumed atnegative electrode.

    Charged section Uncharged section

    Electrode

    1-1-1-1- 2222-2-2-2-2 Manufacturing Processes ofManufacturing Processes ofManufacturing Processes ofManufacturing Processes of

    CADNICA BatteriesCADNICA BatteriesCADNICA BatteriesCADNICA Batteries In order to guarantee the performance character-

    istics which a sealed sintered Nickel-Cadmium cell

    should possess, its manufacturing processes are very

    sophisticated and consist of many stages, A sintered

    plate, for example, is processed as follows to

    guarantee the critical quality needed to maintain the

    excellent performance of CADNICA batteries.

    First of all, nickel powder, which is very small in

    apparent specific gravity and large in specific surface

    area, is mixed with a thickening agent and water

    which in turn is applied on both faces of a core

    substance, such as thin nickel-plated steel plate,

    dried, and then sintered in reducing atmosphere so

    as to produce a sintered base plate of 80 to 85

    porosity, and 0.4 to 0.8mm thickness. The quality of

    this plate, which supports active materials, has great

    bearing upon the performance characteristics of

    sealed cell to be manufactured.

    In the next stage, active materials, which are

    produced from nickel and cadmium salts and which

    are insoluble in water, are loaded in the plate. This

    process is most important because the characteristics

    of the plate are determined in this stage. At Sanyo,

    this process is controlled with great care and

    constant improvements have been made for better

    results.

    The active materials are then reactivated and

    washed clean before the electrodes are wound in a

    roll, being isolated from each other by a porous

    separator. I n the final process, they are assembled

    into a cell and are made ready to undergo strict

    inspections prior to shipment form the factory.

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    1-1-1-1- 2222-3-3-3-3 Structural Designs of CADNICAStructural Designs of CADNICAStructural Designs of CADNICAStructural Designs of CADNICA Sanyo CADNICA batteries range in type from

    standard batteries to fast-charge batteries, or high

    temperature batteries for exclusive use as well as in

    capacity from 45mAh to 20 Ah to meet diverse user

    requirements. Though each type has its own

    structural design according to its required

    performance, the basic structural design is identical.

    Fig.1-2 illustrates the internal view of a CADNICA

    battery where the electrodes are very thin sinteredplates wound compactly in a roll and insulated from

    each other by a porous separator. Almost the entire

    room inside the cell casing is occupied by this roll so

    that energy efficiency as well as charge/discharge,

    and temperature characteristics are raised to the

    highest possible levels. The cell casing is made of

    solid steel.

    Although Sanyo CADNICA batteries are designed to

    completely recombine gas generated within their

    casings, they have a gas release vent, as illustrated

    in Fig.1-3, which opens automatically and releases

    excessive pressure when the internal gas pressure

    increases. Then it is resealed so that the battery can

    be used again. F urthermore, because Sanyos origi-

    nal current collector is employed for both the positive

    and negative tabs(some models excepted), internal

    impedance is extremely small and excellent

    characteristics are exhibited, even under high-rate

    discharge conditions.

    Fig.1-2:Fig.1-2:Fig.1-2:Fig.1-2: Structural DesignStructural DesignStructural DesignStructural Design of CADNICAof CADNICAof CADNICAof CADNICA

    BatteryBatteryBatteryBatteryElectricWelding

    Positive tab

    Negativeelectrode

    Separator

    Positive electrode

    Spring

    Seal plate

    Rubber plate

    Positive current collector

    Separator

    Positiveelectrode

    Negativeelectrode

    Enlargement

    Positive cap

    Cover plate

    Gasket

    Casing

    Negativetab

    Fig.1-3:Fig.1-3:Fig.1-3:Fig.1-3: Structural Design of GasStructural Design of GasStructural Design of GasStructural Design of Gas

    Release VentRelease VentRelease VentRelease VentPositive cap

    Seal plate

    Rubber plate

    Spring

    Gasket

    Over plate

    Casing

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    2ChargeChargeChargeCharge

    CharacteristicsCharacteristicsCharacteristicsCharacteristics2-1 Outline of Charge

    Characteristics

    2-2 Charge Efficiency

    2-3 Cell Temperature

    during Charge

    2-4 Internal Gas Pressure

    during Charge

    2-5 Cell Voltage

    2-12-12-12-1 Outline of ChargeOutline of ChargeOutline of ChargeOutline of Charge

    CharacteristicsCharacteristicsCharacteristicsCharacteristics

    CADNICA batteries should be charged with

    constant or quasi-constant current. As illustrated in

    Fig.2-1, the general characteristics of CADNICA

    batteries such as cell voltage, internal gas pressure

    and cell temperature vary during charge, depending

    on charge current and ambient temperature.

    Fig.2-1:Fig.2-1:Fig.2-1:Fig.2-1: Charge CharacteristicsCharge CharacteristicsCharge CharacteristicsCharge Characteristics

    1.0

    1.1

    1.2

    1.3

    1.4

    1.5

    10 12 14 16 18 200

    0.1

    0.2

    0.3

    0.4

    0.5

    0.6

    86420

    10

    0

    20

    30

    40

    50

    C e ll voltag e

    C ell tem pe rature

    Internal ga s pressure

    N -1300S C

    C h arge0.1ItTe m perature20

    As mentioned in Section 1-4 above, the sealed

    structure of CADNICA batteries has been achieved

    by recombining oxygen gas, which is generated at the

    positive electrode during overcharging, at the

    negative electrode. However, since recombining

    capacity is limited, the charge current of each model

    is determined by first calculating the balance of

    oxygen gas generated at the positive electrode

    against the negative electrodes gas recombination

    capability.

    As long as the input rate is kept lower than thespecified value, internal gas pressure during

    charging will stay low and oxygen generation will not

    be excessive even in the late period of charging.

    The fast-charge type of Sanyo CADNICA batteries is

    designed to accelerate oxygen gas recombination,

    permitting a charge rate of 0.3It for some models.

    1 hour charge is also possible with a simple external

    circuit.

    2-22-22-22-2 Charge EfficiencyCharge EfficiencyCharge EfficiencyCharge Efficiency

    Charge efficiency is the term expressing howeffectively input energy is used for charging the

    active materials into a useful, dischargeable form as

    against total input energy and can be defined as

    follows:

    Charge Efficiency()

    ={ }100 Input energy is used to convert the active materialsinto a charged form, and the side reactions togenerate oxygen gas, etc. Fig.2-2 shows thecorrelations of input energy to the output capacity,

    Discharge CurrentDischarge

    Time to D ischar ge E nd Vol tageCharge CurrentCharge Time100

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    and the charge input to charge efficiency when acompletely discharged cell is charged at the rate of0.1It. The figures given for charge input anddischarge capacity are shown as a percentage ofnominal battery capacity. Charge efficiency variesconsiderably in the course of charging as seen in the

    figure. The dotted line indicates an ideal cell of 100

    charge efficiency.

    In area, of the charts below, electric energy is

    mainly consumed for the conversion of activematerials in the electrode into a chargeable form.

    Therefore, charge efficiency is low at this stage. I n area, which marks the middle of the charging

    process, charging is carried out in a near ideal state,with almost all of the input energy used for theconversion of active materials.

    In area , the cell approaches the state of full

    charge. There the input energy is used for thereaction which generates oxygen gas. The chargeinput is lost and consequently charge efficiencydecreases.

    Fig.2-2:Fig.2-2:Fig.2-2:Fig.2-2: Charge EfficiencyCharge EfficiencyCharge EfficiencyCharge Efficiency

    20

    0

    40

    60

    80

    100

    120

    140

    200180160140120100806040200

    N -1300 S C

    C harge0.1ItD ischarge0.2It,E .V .=1 .0VTe m perature20

    20

    0

    40

    60

    80

    100

    200180160140120100806040200

    23

    1

    100%

    E fficien cyLine

    Charge efficiency depends on charge rate. Fig.2-3 is

    a chart on the correlations existing between the

    charge input and the output capacity, as functions of

    charge rate. The chart shows that the charge

    efficiency as well as the output capacity is lower at a

    lower charge rate.

    Be sure to charge within the current range specified.When charging is performed out of the specified

    current range, charging efficiency is reduced and the

    battery cannot be fully charged.

    Fig.2-3:Fig.2-3:Fig.2-3:Fig.2-3: Charge EfficiencyCharge EfficiencyCharge EfficiencyCharge Efficiency vsvsvsvs

    Charge RateCharge RateCharge RateCharge Rate

    0.01It

    0.02It

    0.033It0.1It1It

    N -1300SC

    20

    0

    40

    60

    80

    100

    120

    140

    200180160140120100806040200

    Tem p20

    Charge efficiency also depends on ambient

    temperature during charge. F ig.2-4 illustrates the

    correlations between charge input and discharge

    capacity, using the ambient temperature as a

    parameter. It is noted that there is a slight decrease

    in cell capacity in the high temperature range due to

    a fall in potential for oxygen gas generation at the

    positive electrode. This decrease in cell capacity is a

    temporary phenomenon and the cell capacity will berecovered when charged at normal temperature.

    Fig.2-5 illustrates the cell capacity vs ambient

    temperature.

    Fig.2-4:Fig.2-4:Fig.2-4:Fig.2-4: Charge EfficiencyCharge EfficiencyCharge EfficiencyCharge Efficiency vs Ambientvs Ambientvs Ambientvs Ambient

    TemperaTemperaTemperaTemperaturetureturetureN -1300S C

    200

    40

    20

    0

    40

    60

    80

    100

    120

    140

    200180160140120100806040200

    C h arge0.1It

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    Fig.2-5:Fig.2-5:Fig.2-5:Fig.2-5: Discharge CapacityDischarge CapacityDischarge CapacityDischarge Capacity vs Ambientvs Ambientvs Ambientvs Ambient

    TemperatureTemperatureTemperatureTemperature

    20

    0

    40

    60

    80

    100

    3020100 40 50 60

    N -1300 S C

    C harge0.1It,0.033It16 0

    D ischarge0.2It,E .V .=1 .0VTe m p erature during discharge20

    0.1It

    0.033ItR ate

    The charge efficiency depends largely on charge rate

    and ambient temperature; therefore the appropriate

    type of CADNICA battery should be selected

    according to the operating requirements.

    2-32-32-32-3 Cell TemperatureCell TemperatureCell TemperatureCell Temperature

    during Chargeduring Chargeduring Chargeduring Charge Though charging reaction in CADNICA batteries is

    in itself endothermic, cell temperature changes very

    little during the initial and intermediate steps of

    charging and is compensated by heat generated by

    internal resistance. Input energy during overcharge

    is converted to heat energy which is generated

    through gas recombination reaction; therefore the

    cell temperature rises. The following factors may

    cause cell temperature to rise:

    (1) Charge current

    (2) Cell design

    (3) Design of battery, (shape, number of cells, etc.)(4) Ambient condition, (temperature, ventilation,

    etc.)

    F ig.2-6 il lustrates the correlation cell temperature

    rise vs charge current with respect to different types

    of batteries. Here generated heat increases with

    charge current, and so does the value of temperature

    rise which also depends on battery type in proportion

    to its size. The battery arrangement or the thermal

    conductance of casing materials becomes important

    for battery assemblies where the closely packed

    arrangement, or the poor thermal conductance of

    casing materials, causes a larger temperature rise.

    Any battery should be charged at a normal ambient

    temperature, and the charging conditions should be

    carefully selected after due consideration to the heat

    generation of cells. The fast-charge batteries are

    controlled according to generated heat during over-

    charge, so the investigation of heat generation

    becomes more significant. Details on this subject may

    be found in paragraph 6-2.

    Fig.2-6:Fig.2-6:Fig.2-6:Fig.2-6: ChargeChargeChargeCharge Current and CellCurrent and CellCurrent and CellCurrent and Cell

    Temperature RiseTemperature RiseTemperature RiseTemperature Rise

    Note: Measured With Single Cell

    2

    6

    8

    10

    12

    14

    16

    18

    20

    0.2 0.3 0.4 0.50.100

    4

    C harge Input200Tem p20

    KR -7000F

    N -1300SC

    N -600AA

    KR -4400D

    2-42-42-42-4 Internal Gas PressureInternal Gas PressureInternal Gas PressureInternal Gas Pressure

    during Chargeduring Chargeduring Chargeduring Charge

    In CADNICA batteries, oxygen gas generated

    during overcharge is recombined in the sealed cell.

    When continuing charging with the specified cur-rent,

    the internal gas pressure achieves a balance

    according to the gas generation and recombination

    rate.

    Fig.2-7 shows changes in internal gas pressure

    when a newly produced cell is tested by varying the

    charge input after the onset of overcharge. Oxygen

    gas is generated in an amount proportionate to the

    charge current on overcharge and causes the internal

    gas pressure to build up.

    Fig.2-7:Fig.2-7:Fig.2-7:Fig.2-7: Overcharge Current and InternalOvercharge Current and InternalOvercharge Current and InternalOvercharge Current and Internal

    Gas Pressure at EquilibriumGas Pressure at EquilibriumGas Pressure at EquilibriumGas Pressure at Equilibrium

    0.2

    0.6

    0.8

    1.0

    0.2 0.3 0.4 0.50.1

    0.4

    Te m p20

    N -1300S C

    00

    The internal gas pressure tends to increase with

    lower ambient temperature as shown in F ig.2-8. Thegas recombination rate at the negative electrode

    decreases with lower ambient temperature so that

    the charge current should be accordingly lower.

    Fig.2-9 shows a sample of recommended charging

    current at low temperatures.

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    Fig.2-8:Fig.2-8:Fig.2-8:Fig.2-8: CharCharCharCharge Temperature andge Temperature andge Temperature andge Temperature and

    Internal Gas PressureInternal Gas PressureInternal Gas PressureInternal Gas Pressure

    N -1300S C

    N -1300 S C R

    C h arge0.3It

    0.2

    0

    0.6

    1.0

    20 30 40100

    0.4

    0.8

    KR -1300S C

    C h arge0.1It

    0.6

    1.0

    20 30 40100

    0.4

    0.8

    0.2

    0

    Fig.2-9:Fig.2-9:Fig.2-9:Fig.2-9: Ambient Temperature andAmbient Temperature andAmbient Temperature andAmbient Temperature and

    Recommended Charge CurrentRecommended Charge CurrentRecommended Charge CurrentRecommended Charge Current

    Note: For some models, charge currents differ from the

    figures shown above.

    0-10-200

    0.02

    0.1

    0.2

    10 20 30

    2-52-52-52-5 Cell VoltageCell VoltageCell VoltageCell Voltage

    The cell voltage of Sanyo CADNICA batteries varies,

    depending on charge current, ambient temperature

    during charge, cell design and other factors.

    The cell voltage increases in the course of charging,

    and drops slightly in the end to its equilibrium valuebecause of heat generation within the cell, as shown

    in Fig.2-1. F ig.2-10 illustrates the cell voltage as a

    function of charge current where charge voltage goes

    higher with an increase in charge input, accompanied

    by increased internal resistance and polarization

    values inside the cell.

    The cell voltage also depends on ambient tempera-

    ture, as shown in Fig.2-11, where the temperature

    rise results in voltage decrease.

    As the temperature climbs, there is a decrease in

    internal resistance as well as in oxygen gas

    generation potential. During charge at the 0.1It rate,

    charge voltage fluctuates within a range of 3.0 to

    4.0mV/degree. Fig.2-12 illustrates the range of cell

    voltage at the end of charging in relation to ambient

    temperatures at the charge rate of 0.1It.

    Fig.2-10:Fig.2-10:Fig.2-10:Fig.2-10: Charge Current and CellCharge Current and CellCharge Current and CellCharge Current and Cell

    VoltageVoltageVoltageVoltage

    20 40 60 80 100 120 140 160 180 200

    1.4

    1.5

    1.6

    N -1300S C

    1.2

    1.10

    1It0.1It0.033It0.02It

    1.3

    20 40 60 80 100 120 140 160 180 200

    1.4

    1.5

    1.6

    1.7

    K R -1300S C

    1.2

    1.10

    0.1It0.033It0.02It

    Te m perature20

    Tem perature20

    1.3

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    Fig.2-11:Fig.2-11:Fig.2-11:Fig.2-11: Ambient Temperature and CellAmbient Temperature and CellAmbient Temperature and CellAmbient Temperature and Cell

    VoltageVoltageVoltageVoltage

    20 40 60 80 100 120 140 160 180 200

    1.4

    1.5

    1.6

    1.7N -1300SC

    1.2

    1.10

    0

    20

    45

    1.3

    charge0.1It

    Fig.2-12:Fig.2-12:Fig.2-12:Fig.2-12: Ambient Temperature and CellAmbient Temperature and CellAmbient Temperature and CellAmbient Temperature and Cell

    VoltaVoltaVoltaVoltage at the End of Chargingge at the End of Chargingge at the End of Chargingge at the End of Charging

    0 10 20 30 40 50 601.1

    1.2

    1.3

    1.4

    1.5

    1.6

    1.7

    1.8

    cha rge0.1It

    KR -1300S C

    N -1300S C

    CellVoltageat

    theEndofCharging

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    3DischargeDischargeDischargeDischarge

    CharacteristicsCharacteristicsCharacteristicsCharacteristics3-1 Outline of Discharge

    Characteristics

    3-2 Internal Resistance

    3-3 Discharge Capacity

    3-4 Polarity Reversal

    3-13-13-13-1 Outline of DischargeOutline of DischargeOutline of DischargeOutline of Discharge

    CharacteristicsCharacteristicsCharacteristicsCharacteristics

    Discharge voltage and cell capacity (self-sustaining

    discharge duration) are the units commonly employ-

    ed to express the discharge characteristics of

    batteries. The voltage of a Nickel-Cadmium cell

    remains almost constant at 1.2V until most of its

    capacity is discharged. Discharge voltage dropsvery little even during high current discharge, and a

    great amount of current more than 100It can be

    discharged in a very short time.

    The capacity of CADNICA batteries is defined in

    terms of the time from the start to the end of

    discharge multiplied by the discharge current, where

    the unit is Ah, (ampere hours), or mAh, (milliampere

    hours).

    The capacity given for each type of CADNICA

    battery is specified by a 5 hour rate at 0.2It discharge

    current. However, the actual capacity depends on

    discharge current and ambient temperature.

    Fig.3-1 compares the discharge characteristics of anordinary dry cell and a CADNICA battery. The cell

    voltage decreases with discharge in an ordinary dry

    cell , while the CADNICA battery exhibits an

    excellent characteristics of constant discharge

    voltage due to its low internal resistance, and less

    variation during discharge.

    Fig.3-1:Fig.3-1:Fig.3-1:Fig.3-1: Discharge CharacteristicsDischarge CharacteristicsDischarge CharacteristicsDischarge Characteristics

    of Ordinary Dry Cell andof Ordinary Dry Cell andof Ordinary Dry Cell andof Ordinary Dry Cell and

    CADNICA BatteryCADNICA BatteryCADNICA BatteryCADNICA Battery

    0

    20

    300

    400

    500

    600

    700

    1.0

    1.2

    1.4

    1.6

    10 2 3 4 5 6

    D ischarge300m A

    Tem p20D ischarge voltage o f C A D N IC A

    battery(N -200 0C )

    D ischarge voltageof dry cell(R14 )

    Internal resistance o f dry ce ll(R14 )

    Internal resistance of C A D N IC A b attery (N -2000C )

    0.6

    0.8

    0.4

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    3-23-23-23-2 Internal ImpedanceInternal ImpedanceInternal ImpedanceInternal Impedance

    As mentioned previously, the discharge voltage of a

    CADNICA battery remains stable for a long duration.

    One of the factors which explain this is the batterys

    low internal impedance. The low internal impedance

    is due mainly to the use of thin and large surface

    sintered nickel plates which exhibit excellent

    conductivity. and a thin separator of nonwoven fabric

    which exhibits excellent electrolyte retention.

    Internal impedance is a key parameter for the

    discharge characteristics of batteries.

    3-2-13-2-13-2-13-2-1 Components of InternalComponents of InternalComponents of InternalComponents of Internal

    ResistanceResistanceResistanceResistance Discharge voltage of CADNICA batteries is expres-

    sed as below:

    V = E0 IZ

    where: E0= no load or open circuit voltage

    I =discharge current

    Z = internal resistance

    This equation confirms that discharge voltage is

    higher with lower internal resistance. Internal

    resistance consists of 3 resistive components: Z = r +

    r + jX. I n this equation, r represents ohmic

    resistance due to conductivity or structure of current

    collector, electrode plates, separator, electrolytes, etc.

    The rdenotes the resistance due to polarization,

    when polarization is a phenomenon where the

    electrode potentials value deviates from the equilib-

    rium one when current circulates through the

    electrodes. Ohmic resistance r is independent of

    current, while polarization r varies in acomplicated way according to current. r also

    value with time and needs several seconds to reach

    its equilibrium value. Thus r is negligible for

    discharge pulse duration of a few milliseconds. jX

    denotes reactance for example, the resistance caused

    by alternating-current wave.

    The reactance is very low at normal charge/dis-

    charge. Thus, discharge voltage during discharge is

    written as below:

    V = E0I(r+r) (during discharge)

    V = E0Ir (momentary, after start of

    discharge and for dischargepulses of a few milliseconds.)

    The internal impedance of a cell varies due to

    various factors. As shown in F ig.3-2, the internal

    impedance of CADNICA batteries undergoes almost

    no change during discharge from the state of full

    charge to the point where 90% of its capacity has

    been dissipated. After that point it increases due to

    the conversion of active materials in the electrode

    plates into hydroxides, which tend to lower electrical

    conductivity.

    Fig.3-3 il lustrates the effect of ambient tempera-

    tures on internal resistance. The internal impedance

    increases as the temperature drops, because the

    conductivity of electrolytes is lower at lower tempe-

    ratures.

    Fig.3-2Fig.3-2Fig.3-2Fig.3-2 Internal Impedance andInternal Impedance andInternal Impedance andInternal Impedance and

    Discharge CapacityDischarge CapacityDischarge CapacityDischarge Capacity16

    14

    12

    10

    8

    6

    4

    2

    00 20 40 60 80 100

    C harge0.1It16H rsD ischa rge0.2It

    Te m p20N -600A A

    N -1300S C

    Fig.3-3:Fig.3-3:Fig.3-3:Fig.3-3: Internal Impedance andInternal Impedance andInternal Impedance andInternal Impedance and

    Cell TempeCell TempeCell TempeCell Temperatureratureraturerature

    20

    Fully charged cell

    N -1300SC

    N -600AA

    0 20 40 60

    16

    14

    12

    10

    8

    6

    4

    2

    0

    3-2-23-2-23-2-23-2-2 Measurements of InternalMeasurements of InternalMeasurements of InternalMeasurements of InternalImpedanceImpedanceImpedanceImpedance There are two methods of measuring internal

    impedance; the direct-current method and the

    alternating-current method. The internal impedance

    of CADNICA batteries is difficult to estimate because

    of its low impedance and complicated variables.

    (1) Direct-current method

    Fig.3-4 illustrates a basic wiring diagram for this

    method. Close the switch Sw and record the changes

    of current and voltage while adjusting the variable-

    resistance Rv. When the change of variable-

    resistance is low, then the voltage change is

    approximated by a straight line; where it drops off

    and gives the value of internal impedance.

    That is, R =

    The internal impedance estimated by the direct-

    current method is equal to r + r, as mentioned

    before, where the polarization term is included, so

    that it varies with the increase in current, or the

    current circulation period.

    V

    I

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    Fig.3-4:Fig.3-4:Fig.3-4:Fig.3-4: Internal Impedance MeasuredInternal Impedance MeasuredInternal Impedance MeasuredInternal Impedance Measured

    by Direct Current Methodby Direct Current Methodby Direct Current Methodby Direct Current Method

    V

    A

    Battery

    SW

    I

    (2) Alternating-current method

    The alternating-current method is used to avoid the

    influence of polarization. The basic circuit for the

    alternating-current method consists of an AC power

    supply circuit and a voltage detection circuit, as

    shown in Fig.3-5.

    The alternating-current impedance is calculated from

    the voltage drop at constant alternating-current

    through a cell as:

    Z =

    The impedance estimated by the alternating-current

    method is equal to r + jX, where the reactance term is

    included, though polarization is negligible.

    Impedance when using AC current varies according

    to current frequency. The technical data of Sanyo

    gives the value estimated by the alternating-current

    method (at 1 KHz) unless otherwise specified.

    Fig.3-5:Fig.3-5:Fig.3-5:Fig.3-5: Measuring Internal ResistanMeasuring Internal ResistanMeasuring Internal ResistanMeasuring Internal Resistancececece

    by Alternating-Current Methodby Alternating-Current Methodby Alternating-Current Methodby Alternating-Current Method

    Battery

    AC ppowersupply circuit

    Voltagedetection circuit

    i

    V

    3-33-33-33-3 Discharge CapacityDischarge CapacityDischarge CapacityDischarge Capacity

    The capacity of CADNICA batteries is derived from

    the discharge current and the time from start to

    finish of discharge. Here the influence of discharge

    end voltage, discharge rate, ambient temperature

    during discharge, etc., on discharge capacity will be

    discussed.

    3-3-13-3-13-3-13-3-1 Discharge End VoltageDischarge End VoltageDischarge End VoltageDischarge End Voltage When estimating battery capacity and discharge in

    actual applications, the discharge end voltage is

    defined as the limiting voltage when a battery is con-

    sidered to have no residual capacity. The standard

    end voltage adopted for CADNICA batteries is 1.0

    V/cell. The end voltage can be 1.1 V/cell, (for signal of

    emergency lamps), or 1.02 V/cell, (for automatic fire

    alarms), according to operational requirements.

    CADNICA batteries have extremely stable voltage

    characteristics during discharge, and the voltage

    drop occurs suddenly at the end of discharge, so that

    the difference in the discharge capacity is minorwhen specified in terms of the end voltage around 1.0

    V/cell. The difference in the discharge time at the 1 It

    rate would be within a range of 1 to 2 minutes

    between the end voltage, 1.0 V/cell and 1.1 V/cell.

    Since the cell voltage drops at high current discharge,

    the energy stored in the battery may not be fully

    discharged with discharge end voltage higher than

    1.0 V/cell.

    v

    i

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    3-3-23-3-23-3-23-3-2 Discharge RateDischarge RateDischarge RateDischarge Rate The discharge capacity of a cell decreases as the

    discharge current increases, as shown in Fig.3-6,

    since the active materials of electrodes are used less

    effectively with higher discharge current. Fig.3-7

    illustrates that the discharge voltage drops as the

    discharge current increases. The reason is an

    increased loss of energy due to internal resistance.

    Compared with other batteries, CADNICA batteries

    have an excellent high current discharge capabilitieswhere the continuous discharge at the rate of 4 I t or,

    in some types, a high current discharge of over 10 It

    is possible.

    Fig.3-6:Fig.3-6:Fig.3-6:Fig.3-6: Discharge Rate andDischarge Rate andDischarge Rate andDischarge Rate and

    Discharge CapacityDischarge CapacityDischarge CapacityDischarge Capacity

    N -1300S C

    0 2 4 6 80

    20

    40

    60

    80

    100

    120

    C harge0.1It16H rs.

    D ischargeE..1.0

    Tem p20

    Fig.3-7:Fig.3-7:Fig.3-7:Fig.3-7: Discharge VoltageDischarge VoltageDischarge VoltageDischarge Voltage

    CharactCharactCharactCharacteristicseristicseristicseristics

    0 20 40 60 80 100 120

    0.8

    1.0

    1.2

    1.4

    8 It 4 It 1 It 0 .2 It

    N -1300SC

    C harge0.1It16 H rs.

    Tem p20

    3-3-33-3-33-3-33-3-3 Ambient TemperatureAmbient TemperatureAmbient TemperatureAmbient Temperature Sanyo CADNICA batteries can be used over a very

    wide temperature range, from. 20 to + 60.

    Though the discharge characteristics will not change

    as the temperature increases, a drop in temperature

    causes internal impedance to be higher, and active

    materials to be less reactive, so that the discharge

    capacity as well as the discharge voltage decreases.

    The tendency is more marked in higher rates of

    discharge. This decrease of discharge capacity is atemporary phenomenon, much like the decrease in

    capacity at high-temperature. Figs.3-8 and 3-9

    illustrate the discharge temperature characteristics

    and the discharge voltage characteristics of

    CADNI CA batteries.

    Fig.3-8:Fig.3-8:Fig.3-8:Fig.3-8: Discharge TemperatureDischarge TemperatureDischarge TemperatureDischarge Temperature

    CharacteristicsCharacteristicsCharacteristicsCharacteristics

    20 0 20 40 600

    20

    40

    100

    N -1300S C

    60

    80

    C harge0.1It16H rs.,20D ischa rgeE..1.0

    0.2It R ate

    1It R ate

    Fig.3-9:Fig.3-9:Fig.3-9:Fig.3-9: Discharge VoltageDischarge VoltageDischarge VoltageDischarge Voltage

    CharacteristicsCharacteristicsCharacteristicsCharacteristics

    0 20 40 60 80 100 120

    0.8

    1.0

    1.2

    1.4

    N -1300S C

    20 0 20 60

    C harge0.1It16H rs.,20

    D isch ag e rate0.2It

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    3-43-43-43-4 Polarity ReversalPolarity ReversalPolarity ReversalPolarity Reversal

    Deep discharge of series connected cells, when

    differences in residual capacity between cells exist,

    may cause one of the cells to reach the state of

    complete discharge sooner then the others. As it

    becomes over-discharged, its polarity is reversed. See

    Fig.3-10 for the discharge voltage curve of the cell on

    forced discharge, including polarity reversal.

    Section of the graph shows the period when

    recharged active materials remain on both positive

    and negative electrodes, with charging voltage at

    normal levels.

    Section shows the period when all the active

    materials on the positive electrode have been

    discharged and hydrogen gas starts to be generated

    on the positive electrode, creating a hydrogen gas

    build up inside the cell. Active materials still remain

    at the negative electrode, however, and discharging

    continues at this electrode. Cell voltage changes

    according to discharge current, but stays about 0.2

    0.4V.

    In section, discharging has been completed at both

    the positive and negative electrode, and oxygen gas

    starts being generated at the negative electrode. I n

    prolonged discharging where this type of polarity

    reversal takes place, gas pressure within the cell

    rises, resulting in operation of the gas release vent.

    This also leads to a breakdown of the balance of the

    charging capacity of the positive and negative

    electrodes, thus prolonged discharge should be

    strictly avoided.

    I f a cell is left connected to a load for a long period of

    time, the cell will eventually become completely

    discharged and its output voltage wil l drop to 0V. Ifthis occurs, the polarity of the positive electrode will

    become negative(0.8V) and electrolyte may easily

    creep. Therefore, avoid leaving a cell connected to a

    load for too long a time.

    Fig.3-10:Fig.3-10:Fig.3-10:Fig.3-10: Polarity ReversalPolarity ReversalPolarity ReversalPolarity Reversal

    P ositive E lectrode

    P ositive E lectrode

    N egative E lectrode

    2 31

    1.0

    0

    1.0

    1.0

    0

    1.0

    DischargeTime

    N egative E lectrode

    P olarity of po sitiveelectrode reve rsed

    P olarity o f bothelectrode reve rsed

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    4StorageStorageStorageStorage

    CharacteristicsCharacteristicsCharacteristicsCharacteristics4-1 General

    4-2 Storage Conditions

    4-3 Items to be Remembered

    for Storage

    4-14-14-14-1 GeneralGeneralGeneralGeneral

    Generally speaking, a loss of voltage and capacity of

    batteries due to self-discharge during storage is un-

    avoidable. With open-type Nickel-Cadmium batteries,

    or manganese dry cells, this self-discharge is less

    notice-able than with CADNICA batteries which

    have a large facing electrode area and a limited

    amount of electrolyte, all of which are completely

    sealed.

    The following 2 factors greatly affect the self-

    discharge of Nickel-Cadmium batteries while stor-

    age:

    (1) Instability of active materials.

    Nickel oxide is thermodynamically unstable at

    its charged state and self-decomposes gradually

    to generate oxygen gas, which in turn oxidizes

    the negative electrode. Thus, the self-discharge

    proceeds.

    (2) Impurities in electrodes or electrolyte.

    A typical example is the self-discharge due to

    nitrate impurities. Nitric ion, NO3, is reduced

    from a negative electrode to nitrous ion, NO2

    which diffuses to a positive electrode, and is

    oxidized. Thus, the self-discharge proceeds.

    The portion of the capacity of CADNICA batteries

    which is dissipated by self-discharge may, however,

    be completely restored when recharged.

    4-24-24-24-2 Storage ConditionsStorage ConditionsStorage ConditionsStorage Conditions

    4-2-14-2-14-2-14-2-1 Storage TemperatureStorage TemperatureStorage TemperatureStorage TemperatureCADNICA batteries can be stored at temperatures

    ranging from 30 to 50 without essential

    deterioration in performance. The organic materials,

    such as gasket or separator, may deteriorate or

    become deformed at high temperatures during

    prolonged storage. Thus, it is recommended that

    CADNICA batteries be stored at temperature below

    35 if there is a possibility of prolonged storage

    surpassing 3 months.

    A decrease in capacity during storage is determined

    mainly by ambient temperature. F ig.4-1 illustrates

    self-discharge characteristics of CADNICA batteries

    stored at 0, 20, 30 and 45.

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    Fig.4-1:Fig.4-1:Fig.4-1:Fig.4-1: Storage CharacteristicsStorage CharacteristicsStorage CharacteristicsStorage Characteristics

    0

    20

    40

    60

    80

    100

    0 1 2 3

    0

    20

    3045

    N series

    C harge0.1It16H rs.D isch arge0.2It,E ..1.0Storage tem peratures0,20,30,45

    0

    20

    30

    45

    KR series

    0

    20

    40

    60

    80

    100

    0 1 2 3

    Storage TimeMonths

    C harge0.1It16H rs.D ischarge0.2It,E ..1.0storagetem peratures0,20,30,45

    Fig.4-2 shows the relationship between ambient

    temperature and the self-discharge current of

    CADNICA batteries, using this graph, the approxi-

    mate self-discharge current can be determined as

    shown by the example.

    Fig.4-2Fig.4-2Fig.4-2Fig.4-2 Self-Discharge Current andSelf-Discharge Current andSelf-Discharge Current andSelf-Discharge Current and

    Ambient TemperatureAmbient TemperatureAmbient TemperatureAmbient Temperature

    1

    2

    3

    5

    710

    2018

    30

    5070

    100

    200

    300

    10 0 10 20 30 40 50

    E xam ple:The self-discha rge current Is of N -600A A at 20is estimated as: Is=(nominal capacity)(self-discharge current ItmA) =(600)(1810-5)(mA)=10810-3(mA) =108(A)

    Fig.4-3 illustrates the capacity recovery characteris-

    tics after prolonged storage at respective tempera-

    tures. The inactivity of active material is increased

    during high-temperature storage, and as a result, the

    capacity recovery time may be longer. As mentioned

    before, it is recommended that CADNICA batteries

    be stored at low temperatures.

    Fig.4-3:Fig.4-3:Fig.4-3:Fig.4-3: Storage Temperature andStorage Temperature andStorage Temperature andStorage Temperature and

    Capacity RecoveryCapacity RecoveryCapacity RecoveryCapacity Recovery

    CharacteristicCharacteristicCharacteristicCharacteristicN -1300SC

    50

    60

    70

    80

    90

    100

    10 2 3 4 5

    S torage a t 20

    Storage a t 35Storage a t 45

    R ecove ry after 2yea rsstorage in discharge state

    C apa city m easu ring cond itions:C harge:0.1It16H rs.D ischarge:0.2 It, E .V .=1 .0VTe m perature:20

    Number of Cycles after Storage

    4-2-24-2-24-2-24-2-2 Battery ConditionsBattery ConditionsBattery ConditionsBattery Conditions CADNICA batteries may be stored in charged or

    discharged state. Fig.4-4 compares the capacity

    recovery characteristics of charged and discharged

    CADNICA batteries after prolonged storage. Though

    the capacity is recovered with a couple of

    charge/discharge cycles in either case, the capacityrecovery of a discharged battery is more quickly

    achieved.

    Due to differences in self-discharge rate, sealed cells

    in a CADNICA assembled battery may have varying

    degrees of available capacity after having been in

    storage for an extended period of time, so they should

    be recharged prior to being returned to service. I f this

    is not done, polarity reversal may occur in some of the

    cells. I t is advisable for prolonged storage that

    batteries be in the discharged state.

    Fig.4-4:Fig.4-4:Fig.4-4:Fig.4-4: Charged StorageCharged StorageCharged StorageCharged Storage vsvsvsvs

    Discharged StorageDischarged StorageDischarged StorageDischarged StorageN -1300 S C

    50

    60

    70

    80

    90

    100

    1 2 3 4 5

    S torage at discharge state

    S torage at charge state

    R eco very after 2ye ars.stored at 35

    Number of Cycles after Storage

    C ap acity m ea suring con ditions:C harge:0.1It16H rs.D isch arge :0.2It, E .V .=1.0VTe m p erature:20

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    4-2-34-2-34-2-34-2-3 Storage periodStorage periodStorage periodStorage period Sanyo CADNICA batteries can be stored indefinitely

    without the deterioration of electrodes, which is often

    observed in lead-acid batteries.

    Fig.4-5 illustrates sample cases concerning the cycle

    characteristics of cells stored for 3, 5 and 10 years

    respectively.

    Even in the case of long-term storage, the cells high

    rate capacity does not significantly decrease and

    superior cycle characteristics are maintained.

    Fig.4-5Fig.4-5Fig.4-5Fig.4-5 Cycle Characteristics AfterCycle Characteristics AfterCycle Characteristics AfterCycle Characteristics After

    Prolonged StorageProlonged StorageProlonged StorageProlonged StorageN -600A A

    0

    60

    20

    80

    40

    1000 200 300 4 00 500

    S torage for 3 years

    S torage for 5 years

    S torage for 10 years

    C apacity m e asu ringcond ition s:C h arge:0.1It16H rs.D ischarge:0.2It,E .V .=1 .0V

    Te m p.:20

    C ycle cond ition s:C harge:0.1It11 H rs.D isch arge :0.7It1H r.Te m p.:20

    100

    Number of Cycles after Storage

    S torage at 20 in discharged state

    4-34-34-34-3 Items to beItems to beItems to beItems to be Remembered forRemembered forRemembered forRemembered for

    StorageStorageStorageStorage

    Though CADN ICA batteries are maintenance-free,and require no supply of electrolytes, or water during

    storage, the following guidelines should be observed

    to make best use of battery capacity:

    (1) Batteries should be completely discharged prior

    to prolonged storage.

    (2) Batteries should be stored at the possible lowest

    temperature. The temperature should never

    exceed +35 for prolonged storage.

    (3) Batteries should be recharged prior to use after

    prolonged storage.

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    5 atteryService Life5-1 G eneral

    5-2 Factors Influencing Service

    Life

    5-3 Sum m ary of Service Life

    5 1 G eneral The service li fe is defined as, The length of time it

    takes a battery to reach a state of wear-out failure,

    where it can no longer drive the necessary load. Herethe wear-out failure denotes the failure during the

    period when the failure rate increases with time due

    to the elements of fatigue, abrasion of aging, and is

    distinguished from the initial failure and the random

    failure, which denote the failure due to errors in

    design/production or unsuitable specifications, and

    accidental failure, between the initial failure and the

    wear-out failure period, respectively.

    Fig.5 1: Failure Rate Curve

    0

    Initial failure period

    R andom failure pe riodW ear-out failurepe riod

    Service Life

    FailureRate

    The wear-out failure of CADNICA batteries is

    classified into 2 types. One is due to an internal short

    circuit caused by changes in active materials and the

    deterioration of organic materials, such as a

    separator. The other is due to the electrolyte drying

    up. In normal charge and discharge cycles no

    electrolyte will leak outside the cell due to CADNICA

    batterys completely sealed structure. A small

    amount of leakage may occur from the safety vent or

    the sealed part if the battery is charged with a

    current higher than specified, overdischarged until

    polarity reversal occurs, or used at extremely

    high/low temperatures. Repeated loss of electrolyte

    will eventually increase internal resistance and

    decrease capacity.

    The service li fe of CADNICA batteries is generally

    considered to terminate when their availablecapacity has been lowered to less than 60% of the

    nominal capacity.

    This rule, however, is not applicable in conditions

    where, depending upon operating requirements, the

    termination point of their service life is set higher or

    lower than the above mentioned level. Shown in

    Fig.5-2 is the number of charge/discharge cycles in

    relation to discharge capacity. CADNICA batteries

    exhibit excellent cycle characteristics where no

    noticeable drop is observed after 500 charge/

    discharge cycles under Sanyo specified conditions.

    In addition, CADNICA batteries exhibit excellentcycle characteristics even for pulse discharge cycle

    applications.

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    ing. As the figures demonstrate, CADNICA batteries

    can be used for extremely long periods on continuous

    charge cycles.

    Fig.5 2: C ycle CharacteristicsN -1300SC

    0

    60

    20

    80

    40

    2000 400 600 800 1000

    C apacity m easuring conditions:C harge:0.1It16H rs.D ischarge:0.2It,E .V.1.0VTe m perature:20

    C ycle condition s:C harge:0.1It11H rs.D ischarge:0.7It1H rs.Te m perature:20

    100

    Number of Cycles

    Fig.5 3: Pulse Discharge C ycleCharacteristics

    N -1300SC

    0

    60

    20

    80

    40

    1000 200 300 400 500

    C ap acity m easuring cond itions:C harge:0.1It16H rs.D ischarge:0.2 It,E .V.1.0VTem p:20

    C ycle condition s:C harge:0.1It16H rs.D ischarge:resistan ce(10It30sec 1It30sec.)20M ins.Tem p:20

    100

    Number of Cycles

    Fig.5 4: C ontinuous Trickle ChargeCycle C haracteristics

    KR-SCH(1.2)

    0

    60

    20

    80

    40

    10 2 3 4 5

    C harge:It/30~6MonthsDischarge:1It,E.V.1.1VTemp:20

    100

    Service Life (Years)

    5 2 Factors Influencing ServiceLife

    5 2 1 C ell Tem perature One of the most important factors affecting the

    service life of a CADNICA battery is ambient

    temperature. F ig.5-5 illustrates an approximate

    relation between ambient temperature and battery

    service life. Generally speaking the optimum

    temperature is room temperature and temperatures

    higher than 40 will deteriorate cell performance.

    Exposure to a high temperature for a short time

    however will not cause permanent damage and will

    recover with a couple of charge/discharge cycles at

    room temperature. The most adverse effects of a

    prolonged rise in cell temperature may be seen as

    damage to organic materials. Used at hightemperatures for a long time, the separator in

    particular is gradually damaged, and its insulation

    function decreases, resulting in internal short circuit.

    Overcharging and continuous charging at high

    temperatures should be avoided. This accelerates

    deterioration of the separator through oxidization

    resulting from oxygen generated at the positive

    electrode during overcharging.

    Fig.5 5: Am bient Tem perature andBattery Service Life

    5

    10

    20

    30

    40

    60

    80

    100

    0 10 20 30 40 50 60

    5 2 2 C harge C onditions The charge current of a CADNICA battery is

    specified according to its design. As long as a

    CADNICA battery is charged at an input rate below

    the specified value, internal gas pressure remains at

    a low level. However, heat generated by gas

    recombination causes a rise in cell temperature.

    When overcharging is repeated often, heat deter-

    iorates the cell and shortens its service life. Charging

    at rates over specified value increases internal gas

    pressure, occasionally causing operation of the gas

    release vent and should be avoided.

    The batteries as standby power sources of

    emergency lights or signal lights, are continuouslycharged with trickle charge current in order to

    maintain a fully charged state Nickel-Cadmium

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    observed in CADNI CA batteries.

    5 2 3 Discharge C onditions Even when fully discharged, a CADNICA battery

    recovers its capacity by charging. Over-discharge hasonly a minor effect on CADNICA batteries compared

    with lead-acid batteries.Depth of dischargeis the

    term used to express percentage wise the capacity

    removed from a battery at the onset of discharge from

    the state of full charge. The number of cycles

    CADNICA batteries can withstand depends on the

    depth of discharge as illustrated in Fig.5-6. When the

    cell is discharged to a greater depth, the number of

    cycles decreases.

    Fig.5 6: Discharge Depth and BatteryService Life10000

    5000

    3000

    2000

    1000

    700

    500

    300

    20010 20 30 40 50 60 70 80 90 1 000

    C harge curren t:0.1It

    C harge input:150% of

    discha rge d capacity

    D ischarged :1It

    Te m perature:20

    NumberofCycles

    Nickel-Cadmium batteries have a memory-effect

    in which the voltage drops by 2 levels during

    discharge after shallow charge/discharge cycles. In

    application when discharge end voltage is highly

    established, apparent decreases in capacity and

    operating voltage are shown. This phenomenon

    doesnt occur after 1 or 2 complete discharge cycles.

    Fig.5 7: M em ory EffectKR- 1100AEL

    0 10 20 30 40 50 60 70

    0.8

    1.0

    1.2

    1.4 Initial

    1st after 100 cycles

    2nd after 100 cycles

    3rd after 100 cycles

    C ycle condition s:

    C harge:0.1It10H rs.

    D ischa rge:1It10M ins.

    Te m perature:45

    D isch arge C ha racteristics Testing C on dition s:

    C harge:0.1It16H rs.

    D isch arge:1It

    Te m perature:20

    The battery performance is hardly affected by the

    discharge frequency during continuous charge of

    reserve power supply, as il lustrated in F ig.5-8, which

    represents the continuous charge cycle characte-ristics in 3, 6 and 12 months.

    Fig.5 8: Discharge Frequency andC ycle Characteristics

    KR-SCH(1.2)

    20

    40

    60

    80

    120

    0.50 1 1.5 2 2.5 3

    3 m onth cycle

    6 m onth cycle

    1 year cycle

    C harge It/303,6,12M onthsD ischarge:1It,E .V .1.1VTem perature:20

    100

    5 3 Sum m ary of Service Life In the preceding paragraphs various factorsaffecting the service life of Sanyo CADNICA batteries

    have been discussed. The conclusion of the discussion

    is that, if they are used under normal operating

    conditions, a very long service life can be expected.

    CADNICA battery life is determined by these factors

    which relate to one another in an intricate manner.

    Thus, it is difficult to predict how long they will

    generally perform well.

    The relevant factors to battery life are summarized

    below:

    Batterycyclelife

    Degradation inelectrode performance

    Variation inelectrolytedistribution

    Deterioration ofconstituents

    Crystal growth inactive materials

    Loss of electrolyte Venting

    Reverse charge

    Charging at ahigher rate thanspecified.

    Overcharge

    Intermittent charge

    High ambienttemperature

    Overcharge

    Rise in internaltemperature(high-ratecharge/discharge)

    High ambient

    temperature

    Extremely low currentdischarge

    Good understanding of these relevant factors will

    assist the designer of battery-powered devices in

    obtaining the longest life, optimum performance, and

    greatest reliability from Sanyo CADNICA batteries.

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    6SpecialSpecialSpecialSpecial

    PurposePurposePurposePurpose

    BatteriesBatteriesBatteriesBatteries6-1 High-Capacity CADNICA

    Batteries

    6-2 Fast-Charge CADNICA

    Batteries

    6-3 High-Temperature

    CADNICA Batteries

    6-4 Heat-Resistant CADNICA

    Batteries

    6-5 Memory-Backup

    CADNICA Batteries

    (CADNICA BACKUP)

    CADNICA Batteries may be used in various fields

    with excellent results as mentioned before. Sanyo has

    designed CADNICA batteries for special purposes

    that concur with necessary requirements, and

    further improve the efficiency of the devices in which

    they are used.

    The basic structural design of CADNICA batteries

    for exclusive use, is the same as that of standard

    CADNICA batteries. The characteristics of

    CADNICA batteries for exclusive use succeedrespective excellence of standard CADNICA batteries.

    CADNICA batteries for exclusive use are by no

    means limited to a particular field, but may be used

    for many purposes.

    6-16-16-16-1 High-Capacity CADNICAHigh-Capacity CADNICAHigh-Capacity CADNICAHigh-Capacity CADNICA

    BatteriesBatteriesBatteriesBatteries

    6-1-16-1-16-1-16-1-1 CharacteristicsCharacteristicsCharacteristicsCharacteristics The growing use of compact and l ightweight

    equipment has rapidly increased the need for a high-capacity battery. In anticipation of this trend, Sanyo

    has developed high-capacity CADNICA batteries

    with approx. a 40-percent higher capacity featuring a

    significant improvement in energy density while

    employing the same manufacturing method used for

    highly-reliable standard CADNICA batteries. They

    can also be charged in as little as one hour.

    6-1-26-1-26-1-26-1-2 Charge CharacteristicsCharge CharacteristicsCharge CharacteristicsCharge Characteristics High-capacity CADNICA batteries are designed forimproved gas recombination in order to facilitate fast

    charging. They are capable of one-hour charging viaV sensor fast charge system.

    Fig.6-1 shows the charge characteristics forV

    sensor fast charging.

    Please refer to Chapter 7-3 for information

    regarding V sensor fast charging.

    Fig.6-1:Fig.6-1:Fig.6-1:Fig.6-1: Charging CharacteristicsCharging CharacteristicsCharging CharacteristicsCharging Characteristics

    0

    0.5

    1.0

    1.5

    0

    50

    40

    30

    20

    10

    10 20 30 40 500

    KR -1800SC E

    1.0

    1.1

    1.2

    1.3

    1.4

    1.5

    1.6

    1.7

    C ell tem perature

    Internal gus p ressure

    C ha rge:1.5It(V=10m V/cell)Temperature:20

    C ell voltag e

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    6-1-36-1-36-1-36-1-3 DischargDischargDischargDischarge Characteristicse Characteristicse Characteristicse Characteristics The discharge voltages of standard CADNICA batt-

    eries show extremely smooth voltage characteristics

    up to the end of the discharge period. High-capacity

    CADNICA batteries share this advantage, and in

    addition, through a significant improvement in

    energy density, they exhibit a capacity 40% greater

    than previous models.

    Fig.6-2 shows the discharge characteristics of high-

    capacity CADNICA batteries, while Fig.6-3 shows therelationship between discharge current and discha-

    rge capacity. As the figures demonstrate, high-

    capacity CADNICA batteries maintain a higher

    capacity than standard CADNICA batteries at low,

    medium or high current discharge levels.

    Fig.6-2:Fig.6-2:Fig.6-2:Fig.6-2: Discharge CharacteristicsDischarge CharacteristicsDischarge CharacteristicsDischarge Characteristics

    0.4

    1.0

    1.2

    1.6

    100 20 3 0 40 5 0 6 0 70

    C ha rge:0.1 It16Hrs.Discharge:1.7ATemperature:20

    Standa rdC adnicaba tteries(N -130 0S C )

    H igh -capacityC adn icaba tteries(KR -1800S C E )

    0.6

    0.8

    1.4

    Fig.6-3:Fig.6-3:Fig.6-3:Fig.6-3: Discharge Current andDischarge Current andDischarge Current andDischarge Current and

    Discharge CapacityDischarge CapacityDischarge CapacityDischarge Capacity

    1.0

    0.8

    0.6

    1.4

    1.2

    2.0

    1.8

    1.6

    42 6 8 10 12 140

    S tanda rdC adnica batteries(N -1300SC )

    H igh -cap acityC ad nica b atteries(KR -1800SC E)

    C harge:0.1It16H rs.

    D ischarge:E.V .1.0V

    Te m perature:20

    6-1-46-1-46-1-46-1-4 Service LifeService LifeService LifeService Life The service li fe of high-capacity CADNICA batteries

    differs according to the conditions of use. The

    manufacturing process for high-capacity CADNICA

    follows that of standard CADNICA batteries, which

    have consistently demonstrated high reliability.

    Therefore high-capacity CADNICA batteries also

    attain a cycle service life equivalent to that of

    standard CADNICA batteries.

    Fig.6-4 shows an example of cycle characteristics

    with V sensor fast charging. It is possible to use

    high-capacity CADNICA batteries for more than 500

    charge/discharge cycles.

    Fig.6-4:Fig.6-4:Fig.6-4:Fig.6-4: Cycle CharacteristicsCycle CharacteristicsCycle CharacteristicsCycle CharacteristicsKR -1800SC E

    0

    60

    20

    80

    40

    1000 200 300 400 500

    Number of Cycles

    C ycle con ditions:C harge:1.5 It( 10m V /cell)D ischarge:1It55M ins.Tem perature:20

    100

    C apa city m easu ringcond ition s:C harge:1.5It( V10m V /cell)D ischarge:1It,E .V .1.0V

    Tem perature:20

    6-26-26-26-2 Fast-Charge CADNICAFast-Charge CADNICAFast-Charge CADNICAFast-Charge CADNICA

    BatteriesBatteriesBatteriesBatteries

    6-2-16-2-16-2-16-2-1 CharacteristicsCharacteristicsCharacteristicsCharacteristics Standard CADNICA batteries require a charging

    period of 14 to 16 hours at a standard charge current

    of0.1It. I n order to meet demands for a faster

    charging speed, fast-charge CADNICA batteries havebeen developed. Designed to facilitate recombination

    of oxygen gas generated at the electrode, they offer

    the following advantages:

    (1) One-hour quick-charge capability

    With the temperature sensor fast-charge system or

    the V sensor fast charge system, charging time

    can be reduced to as little as approx. one hour.

    ForV sensor fast charging and temperature

    sensor fast charging, see chapter 7-3.

    (2) Excellent high current discharge characteristics

    Through the use of Sanyos original highly-efficient

    current collecting method, plus an electrode that

    demonstrates superior discharge characteristics,these batteries possess excellent voltage characteri-

    stics at high rate discharge.

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    6-2-26-2-26-2-26-2-2 Operating Principle of Fast-Operating Principle of Fast-Operating Principle of Fast-Operating Principle of Fast-

    Charge CADNICA BatteriesCharge CADNICA BatteriesCharge CADNICA BatteriesCharge CADNICA Batteries Sanyo CADNICA batteries generate oxygen at the

    positive electrode as the state of full charge is

    approached, according to the following equation, as

    discussed already in 1-4.

    4OH 2H2O+O2+4e (1)

    In the overcharge region, the charging current is

    completely consumed in gas generation. When the

    charge current isaA, oxygen gas is generated at a

    rate of 208 a ml/hr. at 1atm and 20. Generated

    gas is recombined at the negative electrode according

    to the following formulas:

    Cd+1/2O2+H2O Cd(OH)2 (2)

    O2+2H2O+4e 4OH (3)

    Oxygen gas is generated in proportion to the charge

    current so that the oxygen consumption reaction in

    Eqs. (2) and (3)must be accelerated in order to charge

    at a higher current. Otherwise, unconsumed oxygen

    gas increases the internal pressure to such a level

    that the safety vent will operate. As seen from Eqs.

    (2) and (3), the oxygen consumption reaction takes

    place in the 3-phase zone where the 3 phases,

    electrolyte (liquid), oxygen(gas)and electrode(solid),

    come into contact with each other.

    Fast-charge CADNICA batteries are specifically

    designed in terms of electrode structure and

    electrolyte distribution so that a large number of 3-

    phase zones may be formed. This design makes

    possible fast charging over a period of approx. 1 hour.

    With the temperature-sensor fast-charge system,the charging condition is assessed by detecting the

    surface temperature of the battery. The oxygen gas

    recombination reaction at the negative electrode is

    shown by the above Eqs.(2) and (3). Eq. (2) details an

    oxidized reaction of the metal cadmium, which

    results in high heat generation. This heat in turn

    causes an increase in the battery surface

    temperature. Fast-charge CADNICA batteries are

    designed for faster recombination of generated

    oxygen gas and feature improved internal heat

    conductivity, making a quick increase in surface

    temperature possible.

    6-2-36-2-36-2-36-2-3 Charge ChaCharge ChaCharge ChaCharge Characteristicsracteristicsracteristicsracteristics Fig.6-5 shows the charge characteristics of fast-

    charge CADNICA batteries in comparison with

    standard CADNICA batteries. In order to increase

    gas recombination capability, fast-charge CADNICA

    batteries possess a slightly reduced cell capacity.

    Therefore their peak voltages appear earlier during

    the charging cycle.

    Fast-charge CADNICA batteries show lower charge

    voltages at the end of charging due to the ease with

    which heat is generated within the cell, a result of

    their high capability for oxygen gas recombination.

    Fig.6-5:Fig.6-5:Fig.6-5:Fig.6-5: Fast-Charge CharacteristicsFast- Charge CharacteristicsFast- Charge CharacteristicsFast- Charge Characteristics

    0

    10

    20

    30

    40

    50

    60

    70

    C ell voltag eC harge:1.5It

    C ut-off tem perature

    N-1300SCR

    N -1300SC

    Internal gus pressure

    1.0

    1.1

    1.2

    1.3

    1.4

    1.5

    1.6

    0

    0.5

    1.0

    1.5

    20 30 40 50 60100

    C ell tem perature

    The internal gas pressure of a standard CADNICA

    battery cell quickly increases during charging, while

    that of a fast-charge CADN ICA battery stabil izes at

    approx. 5kg/cm2.

    When only gas recombination is taken into

    consideration, fast-charge CADNICA batteries can be

    said to be capable of withstanding overcharging at a

    current level as high as 1.5It. I f overcharging

    continues, however, the cell temperature will

    continue to increase. After a time, it may badly

    damage the battery. I n order to prevent the

    occurrence of this problem, fast charging must be

    suspended after the appropriate amount of time.

    Fig.6-6 shows the relationship between the level of

    overcharge current and the internal gas pressure,

    while Fig.6-7 shows the relationship between the

    ambient temperature during charging and the

    internal gas pressure.

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    Fig.6-6:Fig.6-6:Fig.6-6:Fig.6-6: Overcharge Current andOvercharge Current andOvercharge Current andOvercharge Current and

    Internal Gas PressureInternal Gas PressureInternal Gas PressureInternal Gas Pressure

    1 2 3 4

    1.0

    1.2

    1.4

    1.6

    1.8

    2.0 N -1300 S C R

    0.8

    0.6

    0.4

    0.2

    00

    Te m perature:20

    Fig.6-7:Fig.6-7:Fig.6-7:Fig.6-7: Ambient Temperature andAmbient Temperature andAmbient Temperature andAmbient Temperature and

    Internal Gas PressureInternal Gas PressureInternal Gas PressureInternal Gas Pressure

    10 20 30 40

    1.0

    1.2

    1.4

    1.6

    1.8

    2.0N-1300SCR

    0.6

    0.4

    0.2

    C harge:1.5 It

    00

    0.8

    6-2-46-2-46-2-46-2-4 DischargeDischargeDischargeDischarge CharacteristicsCharacteristicsCharacteristicsCharacteristics Fast-charge CADNICA batteries employ sintered

    plates which exhibit excellent discharge character-

    istics for both the positive and negative electrodes. In

    addition, through the utilization of Sanyos original

    highly-efficient current collecting method which

    demonstrates superior discharge characteristics,these batteries offer an extremely stable discharge

    performance, even at high current levels.

    Fig.6-8 shows an example of discharge characteris-

    tics.

    Fig.6-8:Fig.6-8:Fig.6-8:Fig.6-8: Discharge CharacteristicsDischarge CharacteristicsDischarge CharacteristicsDischarge Characteristics

    0 20 40 60 80 100 120

    N -1300 S C R

    1.2

    1.0

    0.8

    1.4

    0.2It1It4 It8 It

    C ha rge:1.5 It to 45Tem perature:20

    6-2-56-2-56-2-56-2-5 Temperature CharacteristicsTemperature CharacteristicsTemperature CharacteristicsTemperature Characteristics

    One of the greatest features that V-sensor and

    temperature-sensor fast-charge systems offer is the

    capability of achieving stable cell capacity over a

    wide range of temperatures. However, at low temp-

    erature, gas recombination capacity is reduced and

    internal gas pressure can increase to a level that

    adversely affects service life. Therefore, be sure to

    perform fast-charging under the specified tempera-ture. Fig.6-9 shows charge temperature character-

    istics.

    Fig.6-9:Fig.6-9:Fig.6-9:Fig.6-9: Charge TemperatureCharge TemperatureCharge TemperatureCharge Temperature

    CharacteristicsCharacteristicsCharacteristicsCharacteristics

    10 20 30 40 50

    80

    90

    100

    110 N -1300 S C R

    60

    500

    70

    C harge:1.5 It to 45D ischa rge:1It,E .V .1.0V

    6-2-66-2-66-2-66-2-6 Service LifeService LifeService LifeService Life The gas recombination capability does not decline

    even after many cycles. Battery service life does,

    however, differ according to ambient conditions.

    Although the factors affecting the service life of

    fast-charge CADNICA batteries are essentially the

    same as those of standard CADNICA batteries, the

    charging conditions of the two are very different. In

    the case of fast-charge models, the period of

    overcharge from the onset of temperature increase to

    charge cut-off, should be made as short as possible in

    order to ensure a long service life. Therefore the

    following precautions should be observed when

    designing fast-charge control circuits.

    (1) Temperature-sensor fast-charge control

    (a) In the case of assembled batteries that easily

    radiate heat it takes a long time to reach the

    cut-off temperature. Sanyo recommends a

    design under which temperature increases are

    maximized, either by thickening the materialsof the battery case or by utilizing materials

    which feature low heat conductivity.

    (b) Charged with a temperature-sensor system,

    CADNICA batteries tend to be overcharged in

    proportion to the difference between the

    ambient and cut-off temperatures. Decrease

    the setting value of the cut-off temperature

    when using at low temperature.

    (2) V-sensor fast-charge control

    (a) In the case of assembled batteries that easily

    radiate heat, cell voltage decreases gently after

    reaching its peak. Sanyo recommends a design

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    under which temperature increases are

    maxim-ized, especially for CADNICA batteries

    of small capacity.

    (b) The higher theV value becomes, the more

    the battery becomes overcharged. Set theV

    value to 10~20mV per single cell.

    Fig.6-10 shows temperature-sensor fast-charge cycle

    characteristics. Use for more than 500 charge/disch-

    arge cycles is possible.

    Fig.6-11 shows continuous-charge cycle characteris-tics.

    F ig.6-12 shows super-fast-charge cycle characteris-

    tics. Use for more than 500 charge/discharge cycles is

    possible.

    Fig.6-10:Fig.6-10:Fig.6-10:Fig.6-10: Cycle CharacteristicsCycle CharacteristicsCycle CharacteristicsCycle CharacteristicsN -1300SC R

    0

    60

    20

    80

    40

    1000 200 300 400 500

    Number of Cycles

    C ycle conditions:C harge:1.5It to 45D ischarge:1It55M ins.T em perature:20

    100

    C apacity m easurem ent:C harge:1.5It to 45D ischarge:1It,E .V .1.0VTe m perature:20

    Fig.6-11:Fig.6-11:Fig.6-11:Fig.6-11: Continuous-ChContinuous-ChContinuous-ChContinuous-Charge Cyclearge Cyclearge Cyclearge Cycle

    CharacteristicsCharacteristicsCharacteristicsCharacteristicsN -1300 S C R

    Number of Cycles

    0

    60

    20

    80

    40

    100 20 30 40 50

    100

    C apacity m easurem ent:C harge:0.3It5H rs.D isch arge :1It,E .V .1.0VTe m perature:20

    C ycle con dition s:C harge:0.3 It1W eekD isch arge :1It,E .V .1.0VTe m p erature:20

    Fig.6-12:Fig.6-12:Fig.6-12:Fig.6-12: Super-Fast- Charge CycleSuper-Fast-Charge CycleSuper-Fast-Charge CycleSuper-Fast-Charge Cycle

    CharacteristicsCharacteristicsCharacteristicsCharacteristicsN -1300 S C R

    Number of Cycles

    0

    60

    20

    80

    40

    1000 200 300 400 500

    C apacity m easurem ent:C harge:4It15M ins.D isch arge :1It,E .V .1.0VTe m p erature:20

    C ycle con dition s:C harge:4It15 M ins.D isch arge :1It,E .V .1.0VTe m p erature:20

    100

    6-36-36-36-3 High TemperatureHigh TemperatureHigh TemperatureHigh Temperature

    CADNICA BatteriesCADNICA BatteriesCADNICA BatteriesCADNICA Batteries

    6-3-16-3-16-3-16-3-1 Advantages of High TemperatureAdvantages of High TemperatureAdvantages of High TemperatureAdvantages of High Temperature

    CADNICA BatteriesCADNICA BatteriesCADNICA BatteriesCADNICA Batteries Being maintenance-free, and having a high all-

    owance for overcharge, which no other secondary

    batteries have, high temperature CADNICA batteriesare highly suitable for use in emergency lighting. For

    use in this case, the batteries are continuously

    charged with a low current, (trickle-charged), at a

    relatively high temperature, (35 to 45). High

    temperature CADNICA batteries were designed to

    meet necessary requirements for use in high

    temperature situations. Advantages in using high

    temperature CADNICA batteries are:

    (1) Outstanding charge/discharge characteristics at

    high temperature.

    The high temperature CADNICA battery has a

    high trickle-charge efficiency even in tempera-

    ture as high as 35 to 45.(2) Long service life and high reliability.

    The high temperature CADNICA battery shows

    a minor cycle-deterioration even at high

    temperature, and also withstand overcharge,

    ensuring a long service life.

    6-3-26-3-26-3-26-3-2 Operating Principles of HighOperating Principles of HighOperating Principles of HighOperating Principles of High

    Temperature CADNICATemperature CADNICATemperature CADNICATemperature CADNICA

    BatteriesBatteriesBatteriesBatteries The charging of Nickel-Cadmium batteries in

    general becomes more difficult at higher temperature,

    and with lower current. As explained in Chapter 2,

    this is because the charging reaction of active

    material (1), and the oxygen generation reaction (2),

    compete with each other at the positive electrode

    towards the end of charging.

    Ni(OH)2+ OH NiOOH + H2O+e

    (1)

    4OH 2H2O+O2+4e (2)

    When oxygen gas is generated, the charging

    reaction at the positive electrode becomes reluctant

    to proceed. The generation potential of oxygen

    becomes lower with the increase of cell temperature,so that oxygen is generated in the earlier stage. As a

    result, the charge voltage is low, the charge efficiency

    at the electrode deteriorates, and the charge capacity

    becomes lower.

    The high temperature CADNICA battery is made

    with specially designed electrodes and electrolyte, in

    order to maintain a high generation potential of

    oxygen, even at high temperature.

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    6-3-36-3-36-3-36-3-3 Temperature CharacteristicsTemperature CharacteristicsTemperature CharacteristicsTemperature Characteristics The high temperature CADNICA battery guaran-

    tees its outstanding characteristics even in high

    temperature. Fig.6-13 il lustrates cell capacity as a

    function of ambient temperature where the cell

    capacity at 20 is taken as a standard (100%). The

    high temperature CADNICA battery exhibits maxi-

    mum capacity at just over 20. Though its high

    temperature characteristics are much improved as

    compared with those of the standard CADNICAbattery, the high temperature CADNICA battery has

    slightly lower discharge capacity at low temperature,

    as a result of improving its high temperature quality.

    However, the high temperature CADNICA battery

    can withstand a charge at 0, and a discharge at

    20, as well as the standard CADNICA battery, so

    no practical problem exists.

    Fig.6-13:Fig.6-13:Fig.6-13:Fig.6-13: Temperature CharacteristicsTemperature CharacteristicsTemperature CharacteristicsTemperature Characteristics

    50

    80

    90

    110

    100 20 3 0 40 5 0 60 70

    C harge :It/3048H rs.D isch arge :1It,20,E.V.1.1V

    S tandard C A D N IC A

    H igh tem perature

    C A D N IC A

    60

    70

    100

    6-3-46-3-46-3-46-3-4 Charge CharacteristicsCharge CharacteristicsCharge CharacteristicsCharge CharacteristicsThe high temperature CADNICA battery is usually

    used at a trickle-charge of It/20 to It/50. Fig.6-14

    illustrates the trickle-charge voltage characteristicswith I t/30 current. The charge voltage of the high

    temperature CADNICA battery is slightly higher

    than that of the standard CADNICA battery due to

    the improvement of its oxygen generating potential,

    as mentioned in 6-3-2.

    Fig.6-14:Fig.6-14:Fig.6-14:Fig.6-14: Trickle-Charge VoltageTrickle-Charge VoltageTrickle-Charge VoltageTrickle-Charge Voltage

    CharacteristicsCharacteristicsCharacteristicsCharacteristics

    0 2 0 40 60 8 0 1 00 12 0 1 40 16 0 1 80 20 0

    KR -SC H(1.2)

    1.1

    1.5

    1.6

    1.7

    1.2

    1.3

    1.4

    0

    20

    40

    60

    C ha rge:It/30

    6-3-5 Discharge Characteristics6-3-5 Discharge Characteristics6-3-5 Discharge Characteristics6-3-5 Discharge Characteristics The high temperature CADNICA battery has the

    same basic structure as the standard CADNICA

    battery. Thus, its discharge voltage exhibits a flat

    characteristics at the same voltage level as the

    standard CADNICA battery. The high temperature

    CADNICA battery shows improved discharge charac-

    teristics when trickle-charged in high ambient

    temperature. Figs.6-15 and 6-16 illustrate the high

    temperature trickle-charge characteristics, examples

    A and B, 45 characteristics as specified by J IS

    C 8705, respectively.

    The discharge voltage drop often observed in

    Nickel-Cadmium batteries is only slightly detect-ablein CADNICA batteries when charged continuously at

    high temperatures.

    Fig.6-15:Fig.6-15:Fig.6-15:Fig.6-15: High Temperature Trickle-High Temperature Trickle-High Temperature Trickle-High Temperature Trickle-

    Charge CharacteristicsCharge CharacteristicsCharge CharacteristicsCharge Characteristics

    Example AExample AExample AExample A

    Discharge Time( Mins.)

    1.0

    0.8

    1.2

    1.4

    10 20 30 40 50 600

    S tanda rdCAD NICA

    H ightem peratureCAD NICA

    C harge:It/3048H rs.D ischarge:1ItTem p:45

    Fig.6-16:Fig.6-16:Fig.6-16:Fig.6-16: High Temperature Trickle-High Temperature Trickle-High Temperature Trickle-High Temperature Trickle-

    Charge CharacteristicsCharge CharacteristicsCharge CharacteristicsCharge Characteristics

    Example BExample BExample BExample B

    1.0

    0.8

    1.2

    1.4

    10 20 30 400

    S tanda rdCAD NICA

    H igh tem peratureCAD NICA

    C harge:It/3024H rs.D ischarge:1ItTem p:45

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    6-3-66-3-66-3-66-3-6 Service LifeService LifeService LifeService Life The service life of the high temperature CADN ICA

    battery depends largely on the ambient conditions, as

    mentioned in Chapter 5, though expected as over 4

    years under normal conditions. F ig.6-17 il lustrates

    cycle characteristics